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JEE Main
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JEE Main
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Physics
Chapter
Capacitance

JEE Main · Physics · Capacitance

Two identical capacitors have the same capacitance C . One of them...

Two identical capacitors have the same capacitance C.C . One of them is charged to potential V1{V}_{1} and the other to V2.{V}_{2} . The negative ends of capacitors are connected together. When the positive ends are also connected, the decrease in energy of the combine system is

Options

  1. AC4(V12−V22)\dfrac{C}{4} \left({V}_{1}^{2} - {V}_{2}^{2}\right)
  2. BC4(V12+V22)\dfrac{C}{4} \left({V}_{1}^{2} + {V}_{2}^{2}\right)
  3. C\dfrac{C}{4}{\left({V}_{1} - {V}_{2}\right)}^{2}
  4. D\dfrac{C}{4}{\left({V}_{1} + {V}_{2}\right)}^{2}

Correct answer

C. \dfrac{C}{4}{\left({V}_{1} - {V}_{2}\right)}^{2}

Step-by-step solution

Total energy of two identical capacitors before connection.

E1=12CV12+12CV22{E}_{1} = \dfrac{1}{2}C{V}_{1}^{2} + \dfrac{1}{2}C{V}_{2}^{2} .....(i)

When negative end of one capacitor is connected to negative end of other capacitor and positive to positive, then such type of connection is known as parallel connection.

Hence, equivalent capacitance after connection is given by,

Ceq=C+C{C}_{eq} = C + C

Ceq=2C{C}_{eq} = 2C

Common potential, V=TotalchargeTotalcapacitanceV = \dfrac{Totalcharge}{Totalcapacitance}

=Q1+Q2C+C= \dfrac{{Q}_{1} + {Q}_{2}}{C + C}

=CV1+CV22C= \dfrac{C{V}_{1} + C{V}_{2}}{2C}

=V1+V22= \dfrac{{V}_{1} + {V}_{2}}{2}

∴∴ Total energy after connections

E2=12⋅Ceq⋅V2{E}_{2} = \dfrac{1}{2} ⋅ {C}_{eq} ⋅ V^{2}

=12⋅2C(V1+V22)2= \dfrac{1}{2} ⋅ 2C{\left(\dfrac{{V}_{1} + {V}_{2}}{2}\right)}^{2}

=C4(V1+V2)2= \dfrac{C}{4}{\left({V}_{1} + {V}_{2}\right)}^{2}

∴∴ Decrease in energy =E1−E2= {E}_{1} - {E}_{2}

=12CV12+12CV22−C4(V1+V2)2= \dfrac{1}{2}C{V}_{1}^{2} + \dfrac{1}{2}C{V}_{2}^{2} - \dfrac{C}{4}{\left({V}_{1} + {V}_{2}\right)}^{2}

= \dfrac{C}{4} \left[2{V}_{1}^{2} + 2{V}_{2}^{2} - \left({V}_{1}^{2} + {V}_{2}^{2} +2{V}_{1}{V}_{2}\right)\right]<br/><br/> =\dfrac{C}{4}\left[{V}_{1}^{2} + {V}_{2}^{2} -2{V}_{1}{V}_{2}\right] = \dfrac{C}{4}{\left({V}_{1} - {V}_{2}\right)}^{2}
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